2007A&A...464..487K


Query : 2007A&A...464..487K

2007A&A...464..487K - Astronomy and Astrophysics, volume 464487-493 (2007/3-3)

The nature of damped Lyman α and sub-damped Lyman α absorbers.

KHARE P., KULKARNI V.P., PEROUX C., YORK D.G., LAUROESCH J.T. and MEIRING J.D.

Abstract (from CDS):

We present arguments based on the measured abundances in individual damped Lyman α systems (DLAs) and sub-damped Lyman α systems (sub-DLAs), and also the average abundances inferred in large samples of QSO absorption line systems, to suggest that the amount of dust in intervening QSO absorbers is small and is not responsible for missing many QSOs in magnitude limited QSO surveys. While we can not totally rule out a bimodal dust distribution with a population of very dusty, metal rich, absorbers which push the background QSOs below the observational threshold of current optical spectroscopic studies, based upon the current samples it appears that the metallicity in QSO absorbers decreases with increase in H I column densities beyond 1019cm–2. Thus the sub-DLA population is more metal rich than the DLAs, a trend which may possibly extend to the non-damped Lyman limit systems (NDLLS). Based on the recently discovered mass-metallicity relation for galaxies, we suggest that most sub-DLAs and possibly NDLLS, are associated with massive spiral/elliptical galaxies while most DLAs are associated with low mass galaxies. The sub-DLA galaxies will then contribute a larger fraction of total mass (stellar and ISM) and therefore metals, to the cosmic budget, specially at low redshifts, as compared to the DLAs.

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Journal keyword(s): quasars: absorption lines - galaxies: ISM - galaxies: abundances

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 QSO J1610+4724 QSO 16 10 09.4242526872 +47 24 44.480114820   19.72 19.22     ~ 48 0
3 QSO J1709+3258 QSO 17 09 09.2840193312 +32 58 03.404994240   19.68 19.40     ~ 38 0

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